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Journal articles on the topic 'Self-flux'

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Author: Grafiati

Published: 25 May 2024

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1

Pistinner, S. L., and D. Eichler. "Self-inhibiting heat flux." Monthly Notices of the Royal Astronomical Society 301, no. 1 (November 1998): 49–58. http://dx.doi.org/10.1046/j.1365-8711.1998.01770.x.

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2

Castaño, Diego J., and Teresa M. Castaño. "Self-inductance and magnetic flux." American Journal of Physics 91, no. 8 (August 1, 2023): 622–28. http://dx.doi.org/10.1119/5.0098417.

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The canonical equation for self-inductance involving magnetic flux is examined, and a more general form is presented that can be applied to continuous current distributions. We attempt to clarify and extend the use of the standard equation by recasting it in its more versatile form.

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3

Morel, J. E., and J. M. McGhee. "A Self-Adjoint Angular Flux Equation." Nuclear Science and Engineering 132, no. 3 (July 1999): 312–25. http://dx.doi.org/10.13182/nse132-312.

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4

Lukin, Vyacheslav S. "Self-organization in magnetic flux ropes." Plasma Physics and Controlled Fusion 56, no. 6 (March 10, 2014): 060301. http://dx.doi.org/10.1088/0741-3335/56/6/060301.

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5

Ga, E. M., D. Son, J. G. Bak, and S. G. Lee. "Drift Self-compensating Type Flux-meter for Automatic Magnetic Flux Measurement." Journal of Magnetics 8, no. 4 (December 1, 2003): 160–63. http://dx.doi.org/10.4283/jmag.2003.8.4.160.

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6

Mints, R. G., and Ilya Papiashvili. "Self-generated magnetic flux inYBa2Cu3O7−xgrain boundaries." Physical Review B 62, no. 22 (December 1, 2000): 15214–20. http://dx.doi.org/10.1103/physrevb.62.15214.

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7

Cademartiri, Ludovico, Alessandra Sutti, Gianluca Calestani, Chiara Dionigi, Petr Nozar, and Andrea Migliori. "Flux-Assisted Self-Assembly of Monodisperse Colloids." Langmuir 19, no. 19 (September 2003): 7944–47. http://dx.doi.org/10.1021/la034485r.

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8

Zhou, Pengbo, Guangtong Ma, Yuke Deng, Xingchao Nie, Yao Zhai, Kang Liu, Han Zhang, and Yongjian Li. "A Contactless Self-Regulating HTS Flux Pump." IEEE Transactions on Applied Superconductivity 30, no. 4 (June 2020): 1–6. http://dx.doi.org/10.1109/tasc.2020.2978787.

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9

Okada, Yohji, Masashi Kitagou, Toru Masuzawa, and Masato Enokizono. "Development of Flux Concentrated type Self-Bearing Motor." IFAC Proceedings Volumes 43, no. 18 (2010): 461–66. http://dx.doi.org/10.3182/20100913-3-us-2015.00010.

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10

Pla, Oscar, and Franco Nori. "Self-Organized Critical Behavior in Pinned Flux Lattices." Physical Review Letters 67, no. 7 (August 12, 1991): 919–22. http://dx.doi.org/10.1103/physrevlett.67.919.

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11

Setina, Emily. "Marianne Moore, Photography, and the Self-in-Flux." English Language Notes 44, no. 2 (September 1, 2006): 275–82. http://dx.doi.org/10.1215/00138282-44.2.275.

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12

Krasnyuk, I. B., and R. M. Taranets. "Self-similar distribution in “giant” magnetic flux creep." Technical Physics 52, no. 10 (October 2007): 1247–51. http://dx.doi.org/10.1134/s1063784207100015.

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13

Riedel, K. S. "Flux coordinates, self-consistent equilibria, and variational principle." Physics of Fluids 31, no. 4 (1988): 890. http://dx.doi.org/10.1063/1.866771.

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14

Peets, D. C., Ruixing Liang, Mati Raudsepp, D. A. Bonn, and W. N. Hardy. "Self-flux growth of single-crystalline Tl2Ba2CuO6+x." Physica C: Superconductivity 460-462 (September 2007): 1335–36. http://dx.doi.org/10.1016/j.physc.2007.04.014.

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15

Hashimoto, Shinobu, Kentaro Hattori, Koji Inoue, Ayuka Nakahashi, Sawao Honda, and Yuji Iwamoto. "Self-flux synthesis and photoluminescent properties of LiAl5O8." Materials Research Bulletin 44, no. 1 (January 2009): 70–73. http://dx.doi.org/10.1016/j.materresbull.2008.04.003.

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16

Ivić, Zoran, Nikos Lazarides, and G. P. Tsironis. "Self-induced transparency in a flux-qubit chain." Chaos, Solitons & Fractals: X 1 (March 2019): 100003. http://dx.doi.org/10.1016/j.csfx.2019.100003.

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17

Cao, Chongde, Wolfgang Löser, Günter Behr, Rüdiger Klingeler, Norman Leps, Hartmut Vinzelberg, and Bernd Büchner. "Self-flux growth of large EuCu2Si2 single crystals." Journal of Crystal Growth 318, no. 1 (March 2011): 1043–47. http://dx.doi.org/10.1016/j.jcrysgro.2010.10.197.

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18

Naumov, N. D. "Self-consistent description of charged-particle flux catastrophes." Doklady Physics 49, no. 9 (September 2004): 508–11. http://dx.doi.org/10.1134/1.1810574.

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19

Wegrzyn, J. "Self‐shielding, non‐fluoride containing, flux‐cored wires." Welding International 10, no. 5 (January 1996): 341–45. http://dx.doi.org/10.1080/09507119609549007.

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20

Kumar, Ravi, S. K. Malik, S. P. Pai, P. R. Apte, R. Pinto, R. Vijayaraghavan, and Dhanajay Kumar. "Self-field-induced flux creep inYBa2Cu3O7−ythin films." Physical Review B 46, no. 9 (September 1, 1992): 5766–68. http://dx.doi.org/10.1103/physrevb.46.5766.

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21

Tripp, Steven L., Rafal E. Dunin-Borkowski, and Alexander Wei. "Flux Closure in Self-Assembled Cobalt Nanoparticle Rings." Angewandte Chemie International Edition 42, no. 45 (November 24, 2003): 5591–93. http://dx.doi.org/10.1002/anie.200352825.

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22

Tripp, Steven L., Rafal E. Dunin-Borkowski, and Alexander Wei. "Flux Closure in Self-Assembled Cobalt Nanoparticle Rings." Angewandte Chemie 115, no. 45 (November 24, 2003): 5749–51. http://dx.doi.org/10.1002/ange.200352825.

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23

KIM, KYUN TAK, and YEONG SIK KIM. "EFFECTS OF COUNTERPART MATERIALS ON WEAR BEHAVIOR OF THERMALLY SPRAYED Ni-BASED SELF-FLUX ALLOY COATINGS." International Journal of Modern Physics B 24, no. 15n16 (June 30, 2010): 3023–28. http://dx.doi.org/10.1142/s0217979210066021.

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This study aims at investigating the wear behavior of thermally sprayed Ni -based self-flux alloy coatings against different counterparts. Ni -based self-flux alloy powders were flame-sprayed onto a carbon steel substrate and then heat-treated at temperature of 1000 °C. Dry sliding wear tests were performed using the sliding speeds of 0.2 and 0.8 m/s and the applied loads of 5 and 20 N. AISI 52100, Al 2 O 3, Si 3 N 4 and ZrO 2 balls were used as counterpart materials. Wear behavior of Ni -based self-flux alloy coatings against different counterparts were studied using a scanning electron microscope(SEM) and energy dispersive X-ray spectroscopy (EDX). It was revealed that wear behavior of Ni -based self-flux alloy coatings were much influenced by counterpart materials.

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24

Kim, Yeong Sik, and Kyun Tak Kim. "Effect of Sliding Speed and Applied Load on the Wear Behavior of Thermally Sprayed Ni-Based Self-Flux Alloy Coating." Key Engineering Materials 353-358 (September 2007): 840–43. http://dx.doi.org/10.4028/www.scientific.net/kem.353-358.840.

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This study aims at investigating the effect of the sliding speed and the applied load on the dry sliding wear behavior of thermally sprayed Ni-based self-flux alloy coating. Ni-based self-flux alloy powders were flame-sprayed onto a carbon steel substrate and then these coatings were heat-treated at temperature of 1000 oC. Dry sliding wear tests were performed using the sliding speeds of 0.2, 0.4, 0.6 and 0.8 m/s and the applied loads of 5, 10, 15 and 20 N. AISI 52100 ball (diameter 8 mm) was used as counterpart material. Wear behavior of Ni-based self-flux alloy coatings was studied using a scanning electron microscope (SEM) and energy dispersive X-ray spectroscopy (EDX). It was revealed that microstructure and wear behavior of the Ni-based self-flux alloy coatings were much influenced by the sliding speed and the applied load.

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25

Yamazaki, Masato, Takashi Kasashima, Katsuya Yamagiwa, Takeshi Mitsuoka, and Kazushige Ohbayashi. "Characteristic Design of Microwave Dielectric Materials by Using Self-Flux Compositions." Key Engineering Materials 301 (January 2006): 109–12. http://dx.doi.org/10.4028/www.scientific.net/kem.301.109.

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In order to improve the sinterability and controllability of dielectric properties, we focused on self-flux composition. In the case of Ba(Mg1/3Nb2/3)O3, we selected Ba(1-b)NbbOd as self-flux system and investigated correlations between Q-factor and the b value. Interestingly, high Q-value was obtained only at the b=0.45. Moreover, the dielectric constant and tf change linearly by the quantity of Ba0.55Nb0.45Od under keeping up high-Q value. As a result, it was indicated that the dielectric properties could be controlled by the assumption of stoichiometric composition and liquid phase consisted by self-flux.

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26

Zhang, Shulong, Mingtao Li, Yilun Yang, Chengchun Zhao, Mingzhu He, Yin Hang, and Yifei Fang. "Effects of the initial flux ratio on CeSb2 crystal growth by a self-flux method." CrystEngComm 23, no. 29 (2021): 5045–52. http://dx.doi.org/10.1039/d1ce00557j.

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Self-flux growth of the single crystal CeSb₂ was studied in detail, and the most suitable growth parameters of CeSb₂ were obtained. The unusual magnetoresistance properties of CeSb₂ were observed and discussed.

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27

Chen, Jia, Jiafan Ye, Guoqing Gou, and Wei Gao. "Rare earth elements in self-shielded flux-cored wires and their effect on the weld toughing of U75V rail steel." International Journal of Modern Physics B 34, no. 01n03 (December 30, 2019): 2040054. http://dx.doi.org/10.1142/s0217979220400548.

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Self-shielded flux-cored wire is a new type of welding material that has the advantages of outdoor and high-efficiency application, and it has been used widely for rail repair. A self-shielded flux-cored wire with high alkalinity and rare earth elements was taken for research, and the microstructure, inclusions, hardness and the impact toughness were studied. Rare earth elements could eliminate the oxygen and sulfur when they were added into the molten pool. The addition amount has been optimized to the range of 4% in the self-shielded flux-cored wire when used for rail repairing.

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28

Zhai, Yao, Pengbo Zhou, Jing Li, Chenzhen Sun, Yuxiao Li, Ling Xiao, Yuke Deng, and Guangtong Ma. "Performance Investigation of Contactless Self-Regulating HTS Flux Pump." IEEE Transactions on Applied Superconductivity 31, no. 5 (August 2021): 1–5. http://dx.doi.org/10.1109/tasc.2021.3073531.

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29

XU ZHENG, ZHAO XIAO-RU, WU WEN-BIN, SUN XUE-FENG, ZHOU GUI-EN, LI XIAO-GUANG, and ZHANG YU-HENG. "GROWTH CHARACTERISTICS OF Bi2Sr2CaCu2Oy SINGLE CRYSTALS USING SELF-FLUX." Acta Physica Sinica 45, no. 9 (1996): 1562. http://dx.doi.org/10.7498/aps.45.1562.

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30

Rudner, Mark S., and Justin C. W. Song. "Self-induced Berry flux and spontaneous non-equilibrium magnetism." Nature Physics 15, no. 10 (July 8, 2019): 1017–21. http://dx.doi.org/10.1038/s41567-019-0578-5.

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31

Krasnyuk, I. B. "Self-similar magnetic structures and magnetic flux “Giant” creep." Technical Physics 52, no. 5 (May 2007): 565–70. http://dx.doi.org/10.1134/s1063784207050052.

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32

Komatsu-Hidaka, Chiharu, and Takeo Takizawa. "Single crystal growth of SrGa2S4by the self-flux method." Japanese Journal of Applied Physics 39, S1 (January 1, 2000): 67. http://dx.doi.org/10.7567/jjaps.39s1.67.

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33

Szyndler, Megan W., and Robert M. Corn. "Self-Assembly of Flux-Closure Polygons from Magnetite Nanocubes." Journal of Physical Chemistry Letters 3, no. 17 (August 10, 2012): 2320–25. http://dx.doi.org/10.1021/jz300931s.

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34

Wen, L. C., H. Y. Hsieh, S. C. Chang, M. Y. Lin, Y. H. Lee, W. P. Su, H. C. I. Kao, et al. "Compact Li-doped Gd2Ti2O7 prepared with LiO0.5 self-flux." Materials Research Bulletin 50 (February 2014): 297–302. http://dx.doi.org/10.1016/j.materresbull.2013.10.050.

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35

Bilal, Adel, Jean-Pierre Derendinger, and Konstadinos Sfetsos. "(Weak) G2 holonomy from self-duality, flux and supersymmetry." Nuclear Physics B 628, no. 1-2 (April 2002): 112–32. http://dx.doi.org/10.1016/s0550-3213(02)00042-1.

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36

Kannan, C. V., S. Ganesamoorthy, D. Rajesh, R. Jayavel, and H. Kimura. "Anisotropic properties of self-flux grown LiB3O5 single crystals." Solid State Communications 136, no. 4 (January 2005): 215–19. http://dx.doi.org/10.1016/j.ssc.2005.07.028.

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37

Machida, Akio, Naomi Nagasawa, Takaaki Ami, and Masayuki Suzuki. "Ferroelectricity ofBi2SrTa2O9Single Crystals Grown by the Self-Flux Method." Japanese Journal of Applied Physics 36, Part 1, No. 12A (December 15, 1997): 7267–71. http://dx.doi.org/10.1143/jjap.36.7267.

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38

Burtsev, V. A., and N. V. Kalinin. "Self-pressed radiating theta discharge with trapped magnetic flux." Plasma Devices and Operations 15, no. 2 (June 2007): 147–58. http://dx.doi.org/10.1080/10519990701322807.

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39

Zhang, Haowei, and Haisheng Fang. "Flux synthesis of LiNi0.5Co0.2Mn0.3O2 via in situ self-oxygenation." Ionics 26, no. 6 (April 24, 2020): 3185–92. http://dx.doi.org/10.1007/s11581-020-03576-8.

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40

Kannan, C. V., S. Ganesamoorthy, C. Subramanian, and P. Ramasamy. "Dielectric properties of self-flux-grown RbTiOPO4 single crystals." physica status solidi (a) 196, no. 2 (April 2003): 465–70. http://dx.doi.org/10.1002/pssa.200305941.

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41

Kliem, B., and N. Seehafer. "Helicity shedding by flux rope ejection." Astronomy & Astrophysics 659 (March 2022): A49. http://dx.doi.org/10.1051/0004-6361/202142422.

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Context. We quantitatively address the conjecture that magnetic helicity must be shed from the Sun by eruptions launching coronal mass ejections in order to limit its accumulation in each hemisphere. Aims. By varying the ratio of guide and strapping field and the flux rope twist in a parametric simulation study of flux rope ejection from approximately marginally stable force-free equilibria, different ratios of self- and mutual helicity are set and the onset of the torus or helical kink instability is obtained. Methods. The helicity shed is found to vary over a broad range from a minor to a major part of the initial helicity, with self helicity being largely or completely shed and mutual helicity, which makes up the larger part of the initial helicity, being shed only partly. Torus-unstable configurations with subcritical twist and without a guide field shed up to about two-thirds of the initial helicity, while a highly twisted, kink-unstable configuration sheds only about one-quarter. The parametric study also yields stable force-free flux rope equilibria up to a total flux-normalized helicity of 0.25, with a ratio of self- to total helicity of 0.32 and a ratio of flux rope to external poloidal flux of 0.94. Results. These results numerically demonstrate the conjecture of helicity shedding by coronal mass ejections and provide a first account of its parametric dependence. Both self- and mutual helicity are shed significantly; this reduces the total initial helicity by a fraction of ∼0.4 − 0.65 for typical source region parameters.

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42

Ramírez, J., and J. R. Sanmartín. "Self-similar expansion of laser plasmas with nonlocal heat flux." Laser and Particle Beams 12, no. 1 (March 1994): 55–64. http://dx.doi.org/10.1017/s0263034600007229.

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A previous hydrodynamic model of the expansion of a laser-produced plasma, using classical (Spitzer) heat flux, is reconsidered with a nonlocal heat flux model. The nonlocal law is shown to be valid beyond the range of validity of the classical law, breaking down ultimately, however, in agreement with recent predictions.

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43

Groza, A. D. "p-polarized nonlinear surface polaritons near the surface of an epsilon-near-zero metamaterial with saturable permittivity." Journal of Nonlinear Optical Physics & Materials 24, no. 02 (June 2015): 1550015. http://dx.doi.org/10.1142/s0218863515500150.

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We study p-polarized nonlinear surface polaritons (NLSP) propagating along the interface of an epsilon-near-zero metamaterial with saturable nonlinearity, very small negative linear permittivity and an optically linear medium. On the basis of the exact solution of Maxwell's equations, we investigate the relationship between the NLSP propagation constant and the NLSP energy flux for self-focusing and self-defocusing cases. In both cases, for the chosen value of propagation constant, calculations due to Kerr model lead to the lowest NLSP energy flux compared with the energy flux for metamaterial with saturable permittivity.

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44

Yang, Shuhong, Jun Zhang, Ting Li, and Yang Liu. "Self-cancellation of solar ephemeral regions observed by SDO." Proceedings of the International Astronomical Union 8, S294 (August 2012): 159–60. http://dx.doi.org/10.1017/s1743921313002433.

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AbstractWe study the ephemeral regions (ERs) in the quiet Sun observed by the Solar Dynamics Observatory, and find that they can be classified into two types: normal ERs (NERs) and self-cancelled ERs (SERs). We identify 2988 ERs among which there are 190 SERs, about 6.4% of the ERs. The total self-cancelled flux is 9.8% of the total ER flux. We suggest that the self-cancellation of SERs is caused by the submergence of magnetic loops connecting the dipolar patches, without magnetic energy release.

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45

Lancia, L., C. Fourment, J. Fuchs, J. L. Feugeas, Ph Nicolai, S. Bastiani-Ceccotti, M. Gauthier, et al. "Simultaneous measurement of self-generated magnetic fields and electron heat transport in dense plasma." Laser and Particle Beams 31, no. 4 (September 4, 2013): 653–61. http://dx.doi.org/10.1017/s0263034613000451.

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AbstractThe role of self generated magnetic fields in the transport of a heat wave following a nanosecond laser irradiation of a solid target is investigated. Magnetic fields are expected to localize the electron carrying the heat flux but at the same time are affected in their evolution by the heat flux itself. We performed simultaneous measurements of heat wave propagation velocity within the target and magnetic fields developing on the target surface. These were compared to results obtained by numerical magneto-hydrodynamic modeling, including self-generated B fields. The comparison shows that longitudinal heat flow is overestimated in the simulations. Similarly, but most notably, the radial expansion of the magnetic fields is underestimated by the modeling. The two are likely linked, the more pronounced radial drift of B-fields induces a rotation of heat flux in the radial direction, and corresponding longitudinal heat flux inhibition. This suggests the need for improving present modeling of self-generated magnetic fields evolution in high power laser-matter interaction.

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46

Yashiro, Nobuyoshi, Kazuhiko Kusunoki, Kazuhito Kamei, Mitsuhiro Hasebe, Toru Ujihara, and Kazuo Nakajima. "Growth of SiC Single Crystal from Si-C-(Co, Fe) Ternary Solution." Materials Science Forum 527-529 (October 2006): 115–18. http://dx.doi.org/10.4028/www.scientific.net/msf.527-529.115.

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We carried out the growth of single crystalline silicon carbide (SiC) from Si-C-X (X= Co, Fe) ternary solutions. These ternary solutions are expected to show large carbon solubility compared with Si solvent (self-flux) by means of CALPHAD (CALculation of PHAse Diagrams) method. We investigated the growth rate and the polytype of the grown crystal from the ternary solutions. Then we found that the growth rate from the ternary solutions is much larger than that from the self-flux. The growth rate from Si-C-Co (Si-C-Fe) system was about 6mm/hr (12mm/hr) while that from the self-flux was only 2mm/hr. The grown crystal from the ternary solutions is classified into 6H that takes over the seed polytype.

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47

Baggio, Bruno, Giovanni Marzaro, Giovanni Gambaro, Francesco Marchini, Hibbard E. Williams, and Arturo Borsatti. "Glycosaminoglycan Content, Oxalate Self-Exchange and Protein Phosphorylation in Erythrocytes of Patients with ‘Idiopathic’ Calcium Oxalate Nephrolithiasis." Clinical Science 79, no. 2 (August 1, 1990): 113–16. http://dx.doi.org/10.1042/cs0790113.

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1. This study was performed to test the hypothesis that glycosaminoglycans may play an important role in the observed abnormalities in oxalate flux seen in patients with calcium oxalate nephrolithiasis. 2. Oxalate flux rate, erythrocyte membrane glycosaminoglycan content, membrane protein phosphorylation and effect of heparan sulphate on erythrocyte oxalate flux in vitro were studied in control subjects and patients with calcium oxalate nephrolithiasis. 3. In comparison with control subjects, renal stone-formers showed a significantly higher oxalate self-exchange, a lower erythrocyte membrane glycosaminoglycan content and a higher membrane phosphorylation rate. In stone-formers, erythrocyte glycosaminoglycan content correlated inversely with both oxalate flux rate and protein phosphorylation. In vitro, heparan sulphate promoted a significant fall in the rate of oxalate self-exchange. 4. These findings support the hypothesis that a lower erythrocyte membrane content of glycosaminoglycans enhances membrane protein phosphorylation, leading to an increased rate of transmembrane oxalate flux.

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48

Kotelchuk, A. S. "Influence of thermophysical properties of cores of self-shielding flux-cored wires on welding and technological properties." Paton Welding Journal 2016, no. 1 (January 28, 2016): 30–34. http://dx.doi.org/10.15407/tpwj2016.01.04.

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49

Strutynska, N. Yu. "Interaction in self-flux of systems MI2O-P2O5-TiO2-MIIO (MI - Rb, Rb/K, MII - Cu, Zn)." Functional materials 22, no. 2 (June 30, 2015): 269–73. http://dx.doi.org/10.15407/fm22.02.269.

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50

Zhang, Ming Liang, Yong Lu, and Dong Gao. "Study on Flux-Pinned Interaction between High-Temperature Superconductor and Permanent Magnet and Flux-Pinning’s Self-Stability." Advanced Materials Research 291-294 (July 2011): 1251–54. http://dx.doi.org/10.4028/www.scientific.net/amr.291-294.1251.

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Flux pinned effect (FPE) takes place in high-temperature superconductors (HTSC) when being cooled below critical temperature in magnetic field and appears the self-stable with resisting the disturbing and recovering the initial equilibrium position , even in the failure of control, which is ideal for the activities of spacecraft. In order to investigate the special phenomenon, the image-dipole model (IDM) for interaction and spring-damper model (SDM) for system are adopted in this paper. IDM are based on two assumed images and SDM linked with flux-pinned interface is based on virtual spring and damper. Two models effectively deal with the flux-pinning and give some clear expressions. When moving along single orient, this paper demonstrates the pairs’ self-stability based on two models.

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